BACKGROUND OF THE INVENTION
1. Field of the Invention
[0001] The present invention relates to a ceramic composite material which has a high mechanical
strength and an excellent creep resistance in a wide temperature range from room temperature
to high temperature and is suitable to be used as a structural material at a high
temperature.
2. Description of the Related Art
[0002] SiC or Si
3N
4 has been investigated to develop ceramic materials to be used at high temperatures
but is not sufficient in high temperature properties. As an alternative material thereof,
SiC/SiC composite materials produced by chemical vapor impregnation, provided by Societe
Europeene de Propulsion, have attracted attention, at the present are considered to
be the best high temperature structural materials and have been investigated and developed.
The temperature range at which they can be used is reported to be 1400°C or lower.
[0003] Mr. T. Parthasarathy et al. in Journal of the American Ceramics Society Vol. 76,
No. 1, pp29 - 32 (1993) disclosed a composite of alumina and yttrium aluminum garnet
(sometime hereinafter referred to as "YAG") of eutectic Al
2O
3-Y
3Al
5O
12. Mr. Parthasarathy et al. also disclose a method of producing the composite by unidirectionally
melting and solidifying a mixed powder of Al
2O
3 and Y
2O
3 in a crucible.
[0004] It is comprehensible from the description on page 29, right column, lines 9 to 10
and Figs. 1 and 2 of the literature that the composite is polycrystalline and includes
grain boundaries. This is clearly supported from the description "The failure was
usually along the colony boundaries with crack running along the Al
2O
3-YAG interface boundaries". These colony boundaries are shown as portions where the
microstructure is larger than in the other portions in Fig. 2 of the literature.
[0005] This composite material has stresses equivalent to those of sapphire at 1530°C and
1650°C when the strain rate was make constant.
[0006] Moreover, the present inventors confirmed in experiments that the composite disclosed
by Mr. Parthasarathy et al. includes pores or voids in the microstructure and the
mechanical strength of the composite rapidly lowers at high temperature.
[0007] Therefore, the object of the present invention is to provide a ceramic composite
material comprising sapphire, single crystalline α-Al
2O
3, and YAG, which has an excellent mechanical strength and creep behavior from room
temperature to high temperature and significantly improved these properties particularly
at high temperature.
SUMMARY OF THE INVENTION
[0008] The above object is attained in accordance with the present invention by providing
a composite material consisting essentially of single crystal α-Al
2O
3 and single crystal Y
3Al
5O
12.
BRIEF DESCRIPTION OF THE INVENTION
[0009]
Figs. 1 and 2 are X-ray diffraction patterns of the composite material obtained in
Example 1;
Fig. 3 is a photomicrograph of the composite material of Example 1;
Fig. 4 is an X-ray diffraction pattern of the composite material obtained in Comparative
Example 1; and
Fig. 5 is a photomicrograph of the composite material of Comparative Example 1.
DESCRIPTION OF THE PREFERRED EMBODIMENTS
[0010] The term "single crystal" used in the specification means the crystal structure in
which only a diffraction peak from a certain crystal plane of α-Al
2O
3 or Y
3Al
5O
12 is observed in an X-ray diffraction of the composite material.
[0011] Fig. 1 is an X-ray diffraction pattern from a plane perpendicular to the solidification
direction of the ceramic composite material prepared in Example 1, described later,
and Fig. 2 is an X-ray diffraction pattern from a plane declined by about 76° from
the solidification direction of the same ceramic composite material (no diffraction
peak of Al
2O
3 was obtainable from an angle perpendicular to the solidification direction).
[0012] Fig. 1 shows only a peak at 2θ=33.26° corresponding to diffraction from (420) plane
of YAG. Fig. 2 shows only a peak at 2θ=37.78° corresponding to diffraction from (110)
plane of Al
2O
3. These facts clearly indicate that the ceramic composite material of the present
invention consists of single crystal α-Al
2O
3 and single crystal YAG.
[0013] Fig. 4 is an X-ray diffraction pattern from an angle perpendicular to the solidification
direction of the ceramic composite material prepared in Comparative Example 1. Fig.
4 shows diffraction peaks from (110) plane of Al
2O
3 and (420) plane of YAG, as above, as well as the following peaks: for Al
2O
3, diffraction peaks at 2θ=26.62°, 52.7° and 59.78° corresponding to (012), (024) and
(211) planes respectively and for YAG, diffraction peaks at 2θ=18.1°, 27.8°, 29.78°,
36.64°, 38.22°, 41.18°, 46.62° and 60.7° corresponding to (211), (321), (400), (422),
(431), (521) (532) and (651) planes respectively. This X-ray diffraction clearly indicates
that the ceramic composite material obtained in Comparative Example 1 was polycrystalline.
[0014] The fact that the ceramic composite material of the present invention consists of
single crystal α-Al
2O
3 and YAG and is obviously different from the composite materials obtained by Mr. Parthasarathy
et al. and in Comparative Example 1, is also supported by Fig. 3 showing a photomicrograph
of the ceramic composite material obtained in Example 1. In the photomicrograph shown
in Fig. 3, no colony, grain boundary or coarse grain is observed, in contrast to Figs.
1 and 2 of Mr. Parthasarathy et al.'s literature. This photomicrograph corresponds
well to the result of the X-ray diffraction indicating that the ceramic composite
material consists of single crystal α-Al
2O
3 and single crystal YAG.
[0015] Fig. 5 is a photomicrograph of the ceramic composite material obtained in Comparative
Example 1. Fig. 5 shows that the ceramic composite material includes colonies, grain
boundaries or coarse grains, and pores or voids, as shown in Mr. Parthasarathy et
al.'s literature.
[0016] It is proved from comparison between Figs. 1 and 2 and Fig. 4 and comparison between
Fig. 3 and Fig. 5 that the ceramic composite material of the present invention is
a novel composite material consisting of single crystal α-Al
2O
3 and single crystal YAG, different from the composite material disclosed by Mr. Parthasarathy
et al.
[0017] In the ceramic composite material of the present invention, the single crystal α-Al
2O
3 and single crystal YAG form a uniform sea/island structure when a cross-sectional
microstructure is observed. It is not certain but is considered that the sea is single
crystal α-Al
2O
3 and the island is single crystal YAG. The sizes of the sea and islands may be varied
and controlled by selecting the solidification conditions, but are typically in a
range of 10 to 50 µm.
[0018] The amounts of single crystal α-Al
2O
3 and single crystal YAG in the composite material of the present invention can be
varied in ranges of about 20 to 80% by volume of single crystal α-Al
2O
3 and about 80 to 20% by volume of single crystal YAG, by changing the proportion between
the Al
2O
3 and YAG starting powders. The eutectic composition is 55% by volume of Al
2O
3 and 45% by volume of YAG.
[0019] The ceramic composite material of the present invention can be produced; for example,
by the following process.
[0020] A mixed powder of α-Al
2O
3 and Y
2O
3 powders in a ratio for a desired ceramic composite material is prepared by weighing
and mixing. The mixing method is not particularly limited and may be either of a dry
mixing method or a wet mixing method. In a wet mixing method, alcohol such as methanol
and ethanol is generally used as a medium.
[0021] The mixed powder is then heated to a temperature at which both starting powders are
molten, for example, at 1800 to 2500°C, in a conventional furnace, for example, an
arc furnace to melt the mixed powder.
[0022] Subsequently, the melt is charged in a crucible and then unidirectionally solidified
to prepare a ceramic composite material of the present invention. Alternatively, the
melt is once solidified and crushed and the crushed material is then charged in a
crucible and melted and unidirectionally solidified.
[0023] The atmospheric pressure during the melting and solidification is generally 10
-3 Torr or less, preferably 10
-4 Torr or less. The speed of moving the crucible for unidirectional solidification,
i.e., the rate of growth of the ceramic composite material is generally 50 mm/hour
or less, preferably 1 to 40 mm/hour. The control of the conditions other than the
atmospheric pressure and crucible moving speed can be done in the same manner as in
conventional methods.
[0024] If the atmospheric pressure or the crucible moving speed during the melting and solidification
is outside the above ranges, the material may become polycrystal line, pores or voids
tend to appear at colony boundaries, and it is difficult to obtain a composite material
excellent in mechanical strength and creep behavior.
[0025] The apparatus for unidirectional solidification may be a conventional one in which
a crucible is vertically movably mounted in a vertically arranged cylindrical container,
an induction heating coil is disposed around the approximate center position of the
cylindrical container, and a vacuum pump is provided to evacuate the container space.
EXAMPLES
Example 1
[0026] α-Al
2O
3 powder (Sumitomo Chemical Co., Ltd., AKP-30) and Y
2O
3 powder (Shin-etsu Chemical Co., sub-micron type) in a molar ratio of 82% of the former
to 18% of the latter were milled in a wet ball mill using ethanol. The obtained slurry
was dried in a rotary evaporator to remove ethanol.
[0027] The obtained mixed powder of α-Al
2O
3 and Y
2O
3 was charged in a crucible placed in a chamber, in which the atmospheric pressure
was maintained at 10
-5 Torr and the crucible was heated by an induction coil to 1850 to 1900°C to melt the
mixed powder in the crucible. Subsequently, unidirectional solidification was conducted
by descending the crucible at a speed of 5 mm/hour under the above atmospheric pressure
to obtain a ceramic composite material.
[0028] Figs. 1 and 2 show X-ray diffraction patterns of the composite material obtained
from planes perpendicular to and declined by about 76° from the solidification direction
of the composite material. Only a diffraction peak from (420) plane of single crystal
YAG is observed in Fig. 1 and only a diffraction peak from (110) plane of single crystal
α-Al
2O
3 is observed in Fig. 2, which demonstrates that the above composite material consists
of single crystal YAG and α-Al
2O
3.
[0029] Fig. 3 is a photomicrograph of the composite material. Fig. 3 demonstrates that the
composite material does not include any colony or grain boundary, pores or voids do
not exist, and a uniform sea/island structure is formed.
[0030] The mechanical strengths of the composite material are shown in Table 1, where the
three point bending strength and compressive creep property were measured in air.
Comparative Example 1
[0031] The procedures in Example 1 were repeated except that the atmospheric pressure in
the chamber was normal pressure to obtain a ceramic composite material. The X-ray
diffraction pattern and optical microscopic photograph of the obtained composite material
are shown in Figs. 4 and 5.
[0032] Fig. 4 shows diffraction peaks from (012), (024), (110) and (211) planes of Al
2O
3 and diffraction peaks from (211), (321), (400), (420), (422), (431), (521), (532)
and (651) of YAG, indicating that the composite material is a polycrystal. Fig. 5
demonstrates that the composite material includes colony or grain boundary phases
and pores.
[0033] The mechanical strengths of this composite material are also shown in Table 1. Table
1 also includes the mechanical properties of the sapphire fiber from Journal of the
American Ceramic Society Vol. 63, No. 7, pp429 - 435.
Table 1
| |
Example 1 |
Comparative Example 1 |
Sapphire fiber |
| Three point bending strength (MPa) |
|
|
|
| at 1400°C |
490 |
350 |
- |
| at 1500°C |
490 |
320 |
- |
| at 1600°C |
410 |
250 |
- |
| at 1700°C |
370 |
210 |
- |
| Compressive creep strength at 1600°C (MPa): |
|
|
|
| at Strain rate 1 × 10-4sec-1 |
450 |
270 |
280 |
| at Strain rate 1 × 10-5sec-1 |
370 |
210 |
220 |